Integration of III-V heterostructure tunnel FETs on Si using Template Assisted Selective Epitaxy (TASE)

Size: px
Start display at page:

Download "Integration of III-V heterostructure tunnel FETs on Si using Template Assisted Selective Epitaxy (TASE)"

Transcription

1 Integration of III-V heterostructure tunnel FETs on Si using Template Assisted Selective Epitaxy (TASE) K. Moselund 1, D. Cutaia 1. M. Borg 1, H. Schmid 1, S. Sant 2, A. Schenk 2 and H. Riel 1 1 IBM Research Zurich, Switzerland 2 ETH Zurich, Integrated Systems Laboratory IBM Corporation

2 Outline Motivation & background Low power electronics Tunnel FET functionality & SOA Template Assisted Selective Epitaxy Vertical & Lateral approach Experimental P & N-TFET fabrication Electrical characterization Limitations of InAs/Si P-TFETs Analysis of trap contributions Outlook & Summary InAs D it Si CB VB 1

3 Low power electronics InAs Si P tot V 2 C Vdd f active I Leak Vdd leakage Reduce I Leak, Reduce V dd I D (log) V th = I off Slope = 60mV/dec. DV dd MOSFET Steep Slope Device Phase transition Ferro-FET NEMS Tunnel FET 10 µm Out GND In VDD 2 V th V th V dd V dd V GS Steep subthreshold slope can decrease V th to reduce V dd 100 nm W BCB Spin Torque Switch Domain wall switching

4 Tunnel FET functionality Steep slope V dd scaling and low I off Potential to achieve ultra-low power operation source channel Band-to-band-tunneling (BTBT) acts as bandpass filter cutting off the tails of the Fermi distribution SS < 60 mv/dec possible E C filtering of the Fermi function 3

5 How to make a good tunnel switch Increasing Ion l: Electrostatics GAA, EOT scaling, thin body, doping profiles E g, m*: materials based Ge/InAs source on Si, III-V heterostructures GAA Abrupt doping High-k III-V heterostructures Low thermal budget InAs InAs Si GaSb 4 5

6 State of The Art Tunnel FETs Many different implementations (geometry, materials etc.) reported so far Varying potential for: High I on, low SS, integration potential, scalability. InGaAs Air Bridge, Intel (IEDM 2011) s-sinw on SOI (inverters), FZ Julich (IEDM 2013) InGaAs mesa, Penn state (DRC2011) InAs/GaSb mesa, Notre Dame(IEDM 2012) Planar Zn-diffused InGaAs, Tokyo University(IEDM 2013) GaSb/InAs vertical NW Lund (EDL 2016) Vertical Si-Ge NW, IMEC (IEDM 2013) 3D-2D TFET: MoS 2 & Ge, UCSB (Nature 2015)

7 Complementary TFET technologies Challenging for heterojunction TFETs, due to the need for different material combinations for n- and p-channel devices VLSI 2015: Demonstrated p- and n-type InGaAs/GaAsSb TFETs on the same InP substrate use of metamorphic buffer Using TASE we are able to selective grow InAs and GaSb NWs co-planar to each other VLSI 2016: InAs/Si p-tfets and InAs/GaSb n-tfets are implemented on different wafers, using compatible process flows R. Pandey et al., VLSI Symp. (2015) D. Cutaia et al., VLSI Symp. (2016) TASE technology for heterojunction TFETs Development of heterojunction TFET technology: vertical planar Performance and limitations of fabricated TFETs 5

8 Outline Motivation & background Low power electronics Tunnel FET functionality & SOA Template Assisted Selective Epitaxy Vertical & Lateral approach Experimental P & N-TFET fabrication Electrical characterization Limitations of InAs/Si P-TFETs Analysis of trap contributions Outlook & Summary InAs D it Si CB VB

9 Vertical Implementation of TASE α-si SiO 2 Si/α-Si stack Si substrate Etch sacrificial NW MOVPE growth Deposit SiO 2 Open template α-si selective wet etch Large arrays possible dense integration. III-V GaAs as-grown Template stripped 2 um Less flexibility in parameters, L & L i determined by stack. Applications: TFETs, dense integration, photovoltaics 6

10 Horizontal Implementation of TASE Good control over junction placement. Device parameters (L, L i, W, etc.) easily defined by design. Easier fabrication Applications: MOSFETs, TFETs, arbitrary geometry devices, optoelectronics 7

11 Template Assisted Selective Epitaxy (TASE) Growth on any crystalline orientation Stacked nanowires Enables VLSI integration Abrupt junctions Chemical Analysis: EELS, EDX Scalable Technology Arbitrary geometries InSb InAs Courtesy of L. Gignac, IBM Yorktown. Requirement for Steep slope P. D. Kanungo et al. Nanotechnology, 2013, M. Borg et al. Nanoletters, H. Schmid et al. APL 2015, 8

12 Classical devices fabricated using TASE InAs MOSFETs Device: 10 parallel NWs, L G ~ 150 nm, Results: I on = 480 μa/μm (V DS =0.5V) g m = 0.9 ms/μm (V DS =0.5V) Field-effect mobility ~ 500 cm 2 /Vs SS = 250 mv/dec 23x25 nm TASE grown Hall-bar structures Hall measurements (0.1T, RT) n s = IB/qV H = 3.9x10 17 cm 3 electron mobility = 5400 cm 2 /Vs Material allows good device performance 9 H. Schmid et al. APL 2015,

13 Outline Motivation & background Low power electronics Tunnel FET functionality & SOA Template Assisted Selective Epitaxy Vertical & Lateral approach Experimental P & N-TFET fabrication Electrical characterization Limitations of InAs/Si P-TFETs Analysis of trap contributions Outlook & Summary InAs D it Si CB VB

14 Developing our vertical InAs/Si TFET process TEM: L. Gignac, J. Bruley, C. Breslin TASE Scaled diameter Metal ALD Scaled EOT TEOS K. Moselund, EDL H. Riel IEDM D. Cutaia, et al. J-EDS 2015, D. Cutaia, et al. ULIS Transfer to lateral technology flexibility in device processing & complementary TFETs

15 Horizontal TFET fabrication 11

16 Horizontal TFET fabrication 11

17 Horizontal TFET fabrication 11

18 Horizontal TFET fabrication 11

19 Horizontal InAs/Si p-tfets D. Cutaia et al., VLSI Symp

20 Horizontal InAs/gaSb n-tfets 13 D. Cutaia et al., VLSI Symp 2016

21 InAs/Si p-tfet: comparison vertical vs. planar Observations: Ion boosted x50 by EOT scaling (vertical TFETs) Size: 100 nm cross-section 30nm. Horizontal: SS ave much improved 150 mv/dec ~70mV/dec 14

22 Transfer Characteristics 300K P-TFET: I ON =4μA/μm at V GS =V DS =-0.5V, SS~70-80mV/dec., I ON /I OFF ~10 6 N-TFET: I ON =40μA/μm at V GS,ov =3V, V DS =0.5V, SS~1V/dec., I ON /I OFF ~ D. Cutaia et al., VLSI Symp 2016

23 Transfer Characteristics T-sweep Small T-dependence for I D in the ON state Strong SS T dependence P-TFET: SS ave reduced to 55mV/dec. at 150K N-TFET: SS ave reduced to 400mV/dec. at 150K 16 Slide 23

24 SS and g m /I D p-tfet Subthreshold Slope vs. I D : Traps at InAs/Si heterojunction and InAs/High-k interface Switching region limited by TAT g m /I D vs. V GS : Transconductance efficiency peak at 300K 34V -1 Peak shifts to higher I D when reducing T SS improvement 17

25 Diode/Output characteristics P-TFET: No NDR expected for V GS levels used in measurements (-0.5V) due to gate overlap of source. S. Sant, submitted TED 2016 N-TFET: NDR observed on pn and pin diodes with gate metal removed, but not on TFETs 18 D. Cutaia et al., VLSI Symp 2016

26 Outline Motivation & background Low power electronics Tunnel FET functionality & SOA Template Assisted Selective Epitaxy Vertical & Lateral approach Experimental P & N-TFET fabrication Electrical characterization Limitations of InAs/Si P-TFETs Analysis of trap contributions Outlook & Summary InAs D it Si CB VB

27 Effect of generation centers ( traps ) gate oxide Trap-assisted tunneling (TAT) can be seen as multi-phonon-assisted trap-band tunneling or as field-enhanced multi-phonon generation. Contribution from 3 kinds of traps: bulk, hetero interface, gate oxide interface bulk traps traps at hetero interface n-inas Silicon CB oxide interface traps CB intr. VB A. Palma et al., PRB 56, 9565 (1997) n-inas F. Jiménez-Molinos et al., JAP, 91 (8), 5116 (2002) VB 19 A. Schenk et al. ULIS 2015, S. Sant et al., DRC 2016

28 Individual contributions of TAT mechanisms * BTBT T = 300K InAs/ oxide traps InAs/Si traps Only traps at InAs/Si hetero interface can give desired match with the experimental data S. Sant el. al. submitted to IEEE TED 20

29 Dominant mechanism- thermionic emission InAs V GS =0.3V Silicon TAT Therm. emission 300K BTBT TAT bottleneck Therm. emission bottleneck 125K * Low gate bias: thermionic emission is the bottleneck => SS close to thermionic SS. Medium gate bias: thermionic barrier is lowered => TAT becomes bottleneck. High gate bias: BTBT is dominating mechanism 21

30 Traps in InAs/Si TFETs One active trap level per dislocation D it = 1.5x10 13 cm -2 *TEM image - Tomioka et. al. Nano Lett Large lattice mismatch > 11% between Si and InAs. Predictive simulations show highest tolerable dit level ~ 5x10 11 cm -2. Extreme scaling required, or.. Use of lattice-matched material system InGaAs/GaAsSb. Similar requirements on oxide D it levels. 22

31 State-of-the-art TFETs Different designs different merits SS ave scaling below 60 mv/dec in significant I on range still missing 23

32 Summary Introduced tunnel FETs and low-power electronics Demonstrated TASE growth for TFETs and device fabrication. Demonstrated scaled complementary TFETs InAs/Si P-TFET & InAS/GaSb N-TFET Traps at the oxide and hetero interface are currently limiting perfromance. Outlook Optimization of N-TFET (GaSb doping, gate stack) Reduction of defects essential for all TFETs Applications of TASE to new fields: photonics, sensors, 24

33 Thank you for your attention Acknowledgement: MIND group at IBM Research Zurich TEM images: L. Gignac, J. Bruley, C. Breslin, SIMS: Marinus Hopstaken IBM Research Yorktown Support from colleagues and staff at Binnig- Rohrer Nanotechnol. Center Funding: European FP7 Projects 25

III-V Vertical Nanowire FETs with Steep Subthreshold Towards Sub-10 nm Diameter Devices

III-V Vertical Nanowire FETs with Steep Subthreshold Towards Sub-10 nm Diameter Devices III-V Vertical Nanowire FETs with Steep Subthreshold Towards Sub-10 nm Diameter Devices Jesús A. del Alamo, Xin Zhao, Wenjie Lu, Alon Vardi Microsystems Technology Laboratories, MIT E 3 S Retreat September

More information

III-V CMOS: Quo Vadis?

III-V CMOS: Quo Vadis? III-V CMOS: Quo Vadis? J. A. del Alamo, X. Cai, W. Lu, A. Vardi, and X. Zhao Microsystems Technology Laboratories Massachusetts Institute of Technology Compound Semiconductor Week 2018 Cambridge, MA, May

More information

Record I on (0.50 ma/μm at V DD = 0.5 V and I off = 100 na/μm) 25 nm-gate-length ZrO 2 /InAs/InAlAs MOSFETs

Record I on (0.50 ma/μm at V DD = 0.5 V and I off = 100 na/μm) 25 nm-gate-length ZrO 2 /InAs/InAlAs MOSFETs Record I on (0.50 ma/μm at V DD = 0.5 V and I off = 100 na/μm) 25 nm-gate-length ZrO 2 /InAs/InAlAs MOSFETs Sanghoon Lee 1*, V. Chobpattana 2,C.-Y. Huang 1, B. J. Thibeault 1, W. Mitchell 1, S. Stemmer

More information

Vertical InAs/GaAsSb/GaSb tunneling field-effect transistor on Si with S = 48 mv/decade and Ion = 10 A/m for Ioff = 1 na/m at VDS = 0.

Vertical InAs/GaAsSb/GaSb tunneling field-effect transistor on Si with S = 48 mv/decade and Ion = 10 A/m for Ioff = 1 na/m at VDS = 0. Vertical InAs/GaAsSb/GaSb tunneling field-effect transistor on Si with S = 48 mv/decade and Ion = 10 A/m for Ioff = 1 na/m at VDS = 0.3 V Memisevic, E.; Svensson, Johannes; Hellenbrand, Markus; Lind, Erik;

More information

Nanoscale III-V CMOS

Nanoscale III-V CMOS Nanoscale III-V CMOS J. A. del Alamo Microsystems Technology Laboratories Massachusetts Institute of Technology SEMI Advanced Semiconductor Manufacturing Conference Saratoga Springs, NY; May 16-19, 2016

More information

InGaAs MOSFETs for CMOS:

InGaAs MOSFETs for CMOS: InGaAs MOSFETs for CMOS: Recent Advances in Process Technology J. A. del Alamo, D. Antoniadis, A. Guo, D.-H. Kim 1, T.-W. Kim 2, J. Lin, W. Lu, A. Vardi and X. Zhao Microsystems Technology Laboratories,

More information

Device architectures for the 5nm technology node and beyond Nadine Collaert

Device architectures for the 5nm technology node and beyond Nadine Collaert Device architectures for the 5nm technology node and beyond Nadine Collaert Distinguished member of technical staff, imec Outline Introduction Beyond FinFET: lateral nanowires and vertical transistors

More information

III-V CMOS: the key to sub-10 nm electronics?

III-V CMOS: the key to sub-10 nm electronics? III-V CMOS: the key to sub-10 nm electronics? J. A. del Alamo Microsystems Technology Laboratories, MIT 2011 MRS Spring Meeting and Exhibition Symposium P: Interface Engineering for Post-CMOS Emerging

More information

InGaAs MOSFET Electronics

InGaAs MOSFET Electronics InGaAs MOSFET Electronics J. A. del Alamo Microsystems Technology Laboratories, MIT The 17 th International Symposium Physics of Semiconductors and Applications Jeju, Korea, December 7-11, 2014 Acknowledgements:

More information

III-V on Si for VLSI. 200 mm III-V on Si. Accelerating the next technology revolution. III-V nfet on 200 mm Si

III-V on Si for VLSI. 200 mm III-V on Si. Accelerating the next technology revolution. III-V nfet on 200 mm Si III-V on Si for VLSI Accelerating the next technology revolution 200 mm III-V on Si III-V nfet on 200 mm Si R. Hill, C. Park, J. Barnett, J. Huang, N. Goel, J. Oh, W.Y. Loh, J. Price, P. Kirsch, P, Majhi,

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION doi:10.1038/nature11293 1. Formation of (111)B polar surface on Si(111) for selective-area growth of InGaAs nanowires on Si. Conventional III-V nanowires (NWs) tend to grow in

More information

CMOS Scaling Beyond FinFETs: Nanowires and TFETs

CMOS Scaling Beyond FinFETs: Nanowires and TFETs SEMATECH Symposium June 23, 2011 Tokyo Accelerating the next technology revolution CMOS Scaling Beyond FinFETs: Nanowires and TFETs Chris Hobbs, Wei-Yip Loh, Kerem Akarvardar, Paul Kirsch, and Raj Jammy

More information

Towards Sub-10 nm Diameter InGaAs Vertical nanowire MOSFETs and TFETs

Towards Sub-10 nm Diameter InGaAs Vertical nanowire MOSFETs and TFETs Towards Sub-10 nm Diameter InGaAs Vertical nanowire MOSFETs and TFETs J. A. del Alamo, X. Zhao, W. Lu, and A. Vardi Microsystems Technology Laboratories Massachusetts Institute of Technology 5 th Berkeley

More information

Vertical Nanowire InGaAs MOSFETs Fabricated by a Top-down Approach

Vertical Nanowire InGaAs MOSFETs Fabricated by a Top-down Approach Vertical Nanowire InGaAs MOSFETs Fabricated by a Top-down Approach Xin Zhao, Jianqiang Lin, Christopher Heidelberger, Eugene A. Fitzgerald and Jesús A. del Alamo Microsystems Technology Laboratories, MIT

More information

Nanoscale III-V Electronics: from Quantum-Well Planar MOSFETs to Vertical Nanowire MOSFETs

Nanoscale III-V Electronics: from Quantum-Well Planar MOSFETs to Vertical Nanowire MOSFETs Nanoscale III-V Electronics: from Quantum-Well Planar MOSFETs to Vertical Nanowire MOSFETs J. A. del Alamo Microsystems Technology Laboratories, MIT Purdue University, West Lafayette, IN; September 29,

More information

Record Extrinsic Transconductance (2.45 ms/μm at V DS = 0.5 V) InAs/In 0.53 Ga 0.47 As Channel MOSFETs Using MOCVD Source-Drain Regrowth

Record Extrinsic Transconductance (2.45 ms/μm at V DS = 0.5 V) InAs/In 0.53 Ga 0.47 As Channel MOSFETs Using MOCVD Source-Drain Regrowth Record Extrinsic Transconductance (2.45 ms/μm at = 0.5 V) InAs/In 0.53 Ga 7 As Channel MOSFETs Using MOCVD Source-Drain Regrowth Sanghoon Lee 1*, C.-Y. Huang 1, A. D. Carter 1, D. C. Elias 1, J. J. M.

More information

A New Self-aligned Quantum-Well MOSFET Architecture Fabricated by a Scalable Tight-Pitch Process

A New Self-aligned Quantum-Well MOSFET Architecture Fabricated by a Scalable Tight-Pitch Process A New Self-aligned Quantum-Well MOSFET Architecture Fabricated by a Scalable Tight-Pitch Process Jianqiang Lin, Xin Zhao, Tao Yu, Dimitri A. Antoniadis, and Jesús A. del Alamo Microsystems Technology Laboratories,

More information

Scaling of Vertical InAs GaSb Nanowire Tunneling Field-Effect Transistors on Si

Scaling of Vertical InAs GaSb Nanowire Tunneling Field-Effect Transistors on Si Scaling of Vertical InAs GaSb Nanowire Tunneling Field-Effect Transistors on Si Memisevic, Elvedin; Svensson, Johannes; Hellenbrand, Markus; Lind, Erik; Wernersson, Lars-Erik Published in: IEEE Electron

More information

Comparative Study of Silicon and Germanium Doping-less Tunnel Field Effect Transistors

Comparative Study of Silicon and Germanium Doping-less Tunnel Field Effect Transistors IJSTE - International Journal of Science Technology & Engineering Volume 2 Issue 5 November 2015 ISSN (online): 2349-784X Comparative Study of Silicon and Germanium Doping-less Tunnel Field Effect Transistors

More information

FinFET Devices and Technologies

FinFET Devices and Technologies FinFET Devices and Technologies Jack C. Lee The University of Texas at Austin NCCAVS PAG Seminar 9/25/14 Material Opportunities for Semiconductors 1 Why FinFETs? Planar MOSFETs cannot scale beyond 22nm

More information

Self-aligned, gate-last process for vertical InAs nanowire MOSFETs on Si

Self-aligned, gate-last process for vertical InAs nanowire MOSFETs on Si Self-aligned, gate-last process for vertical InAs nanowire MOSFETs on Si Berg, Martin; Persson, Karl-Magnus; Kilpi, Olli-Pekka; Svensson, Johannes; Lind, Erik; Wernersson, Lars-Erik Published in: Technical

More information

III-V Channel Transistors

III-V Channel Transistors III-V Channel Transistors Jesús A. del Alamo Professor Microsystems Technology Laboratories MIT Acknowledgements: Students and collaborators: D. Antoniadis, J. Lin, W. Lu, A. Vardi, X. Zhao Sponsors: Applied

More information

Electrical Characterization and Modeling of Gate-Last Vertical InAs Nanowire MOSFETs on Si

Electrical Characterization and Modeling of Gate-Last Vertical InAs Nanowire MOSFETs on Si Electrical Characterization and Modeling of Gate-Last Vertical InAs Nanowire MOSFETs on Si Berg, Martin; Kilpi, Olli-Pekka; Persson, Karl-Magnus; Svensson, Johannes; Hellenbrand, Markus; Lind, Erik; Wernersson,

More information

Zota, Cezar B.; Lindelow, Fredrik; Wernersson, Lars Erik; Lind, Erik

Zota, Cezar B.; Lindelow, Fredrik; Wernersson, Lars Erik; Lind, Erik InGaAs tri-gate MOSFETs with record on-current Zota, Cezar B.; Lindelow, Fredrik; Wernersson, Lars Erik; Lind, Erik Published in: 6 IEEE International Electron Devices Meeting, IEDM 6 DOI:.9/IEDM.6.7886

More information

Nanometer-Scale InGaAs Field-Effect Transistors for THz and CMOS Technologies

Nanometer-Scale InGaAs Field-Effect Transistors for THz and CMOS Technologies Nanometer-Scale InGaAs Field-Effect Transistors for THz and CMOS Technologies J. A. del Alamo Microsystems Technology Laboratories, MIT ESSDERC-ESSCIRC 2013 Bucharest, Romania, September 16-20, 2013 Acknowledgements:

More information

InGaAs Nanoelectronics: from THz to CMOS

InGaAs Nanoelectronics: from THz to CMOS InGaAs Nanoelectronics: from THz to CMOS J. A. del Alamo Microsystems Technology Laboratories, MIT IEEE International Conference on Electron Devices and Solid-State Circuits Hong Kong, June 3, 2013 Acknowledgements:

More information

Tunneling Field Effect Transistors for Low Power ULSI

Tunneling Field Effect Transistors for Low Power ULSI Tunneling Field Effect Transistors for Low Power ULSI Byung-Gook Park Inter-university Semiconductor Research Center and School of Electrical and Computer Engineering Seoul National University Outline

More information

Vertical Nanowire Gate-All-Around p-type Tunneling Field-Effect Transistor With Si 0.8 Ge 0.2 /Si Heterojunction

Vertical Nanowire Gate-All-Around p-type Tunneling Field-Effect Transistor With Si 0.8 Ge 0.2 /Si Heterojunction 2012 International Conference on Solid-State and Integrated Circuit (ICSIC 2012) IPCSIT vol. 32 (2012) (2012) IACSIT Press, Singapore Vertical Nanowire Gate-All-Around p-type Tunneling Field-Effect Transistor

More information

Reconfigurable Si-Nanowire Devices

Reconfigurable Si-Nanowire Devices Reconfigurable Si-Nanowire Devices André Heinzig, Walter M. Weber, Dominik Martin, Jens Trommer, Markus König and Thomas Mikolajick andre.heinzig@namlab.com log I d Present CMOS technology ~ 88 % of IC

More information

In principle, the high mobilities of InGaAs and

In principle, the high mobilities of InGaAs and 114Conference report: IEDM part 2 Meeting the challenge of integrating III-Vs with deep submicron silicon High-mobility devices based on indium gallium arsenide (InGaAs) channels could benefit the performance

More information

High-Performance Si Nanowire FET with a Semi Gate-Around Structure Suitable for Integration

High-Performance Si Nanowire FET with a Semi Gate-Around Structure Suitable for Integration High-Performance Si Nanowire FET with a Semi Gate-Around Structure Suitable for Integration Soshi Sato 1, Hideyuki Kamimura 1, Hideaki Arai 1, Kuniyuki Kakushima 2, Parhat Ahmet 1, Kenji Ohmori 3, Keisaku

More information

Experimentally reported sub-60mv/dec

Experimentally reported sub-60mv/dec Experimentally reported sub-60mv/dec swing in Tunnel FETs? 1 We considered InAs conventional, lateral transistor architectures: GAA nanowire, Fin FETs FETs (Tri gate) UTB,DG SOI Analysis is not directly

More information

InAs Quantum-Well MOSFET for logic and microwave applications

InAs Quantum-Well MOSFET for logic and microwave applications AWAD June 29 th 2012 Accelerating the next technology revolution InAs Quantum-Well MOSFET for logic and microwave applications T.-W. Kim, R. Hill, C. D. Young, D. Veksler, L. Morassi, S. Oktybrshky 1,

More information

Modeling the Influence of Dielectric Interface Traps on I-V Characteristics of TFETs

Modeling the Influence of Dielectric Interface Traps on I-V Characteristics of TFETs Modeling the Influence of Dielectric Interface Traps on I-V Characteristics of TFETs Jie Min 1, Peter Asbeck UCSD 1 Present address: Global Foundries, Santa Clara, CA Schematic TFET Structures Based on

More information

Parameter Optimization Of GAA Nano Wire FET Using Taguchi Method

Parameter Optimization Of GAA Nano Wire FET Using Taguchi Method Parameter Optimization Of GAA Nano Wire FET Using Taguchi Method S.P. Venu Madhava Rao E.V.L.N Rangacharyulu K.Lal Kishore Professor, SNIST Professor, PSMCET Registrar, JNTUH Abstract As the process technology

More information

Sub-30 nm InAs Quantum-Well MOSFETs with Self-Aligned Metal Contacts and Sub-1 nm EOT HfO 2 Insulator

Sub-30 nm InAs Quantum-Well MOSFETs with Self-Aligned Metal Contacts and Sub-1 nm EOT HfO 2 Insulator Sub-30 nm InAs Quantum-Well MOSFETs with Self-Aligned Metal Contacts and Sub-1 nm EOT HfO 2 Insulator Jianqiang Lin, Dimitri A. Antoniadis, and Jesús A. del Alamo Microsystems Technology Laboratories,

More information

Enabling Power-Efficient Designs With III-V Heterojunction Tunnel FETs

Enabling Power-Efficient Designs With III-V Heterojunction Tunnel FETs Enabling Power-Efficient Designs With III-V Heterojunction Tunnel FETs Moon S. Kim, Huichu Liu, Karthik Swaminathan, Xueqing Li, Suman Datta, and Vijaykrishnan Narayanan The Pennsylvania State University

More information

Transistors for VLSI, for Wireless: A View Forwards Through Fog

Transistors for VLSI, for Wireless: A View Forwards Through Fog Plenary, Device Research Conference, June 22, 2015, Ohio State Transistors for VLSI, for Wireless: A View Forwards Through Fog Mark Rodwell, UCSB Low-voltage devices P. Long, E. Wilson, S. Mehrotra, M.

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 11/6/2007 MOSFETs Lecture 6 BJTs- Lecture 1 Reading Assignment: Chapter 10 More Scalable Device Structures Vertical Scaling is important. For example,

More information

Beyond Transistor Scaling: New Devices for Ultra Low Energy Information Processing

Beyond Transistor Scaling: New Devices for Ultra Low Energy Information Processing Beyond Transistor Scaling: New Devices for Ultra Low Energy Information Processing Prof. Tsu Jae King Liu Department of Electrical Engineering and Computer Sciences University of California, Berkeley,

More information

FinFET vs. FD-SOI Key Advantages & Disadvantages

FinFET vs. FD-SOI Key Advantages & Disadvantages FinFET vs. FD-SOI Key Advantages & Disadvantages Amiad Conley Technical Marketing Manager Process Diagnostics & Control, Applied Materials ChipEx-2014, Apr 2014 1 Moore s Law The number of transistors

More information

Semiconductor Physics and Devices

Semiconductor Physics and Devices Metal-Semiconductor and Semiconductor Heterojunctions The Metal-Oxide-Semiconductor Field-Effect Transistor (MOSFET) is one of two major types of transistors. The MOSFET is used in digital circuit, because

More information

Resonant Tunneling Device. Kalpesh Raval

Resonant Tunneling Device. Kalpesh Raval Resonant Tunneling Device Kalpesh Raval Outline Diode basics History of Tunnel diode RTD Characteristics & Operation Tunneling Requirements Various Heterostructures Fabrication Technique Challenges Application

More information

The Pennsylvania State University. The Graduate School. Department of Electrical Engineering

The Pennsylvania State University. The Graduate School. Department of Electrical Engineering The Pennsylvania State University The Graduate School Department of Electrical Engineering DEVICE CIRCUIT INTERACTIONS FOR STEEP SWITCHING SLOPE DEVICES A Dissertation in Electrical Engineering by Huichu

More information

Design of Tunnel FET and its Performance characteristics with various materials

Design of Tunnel FET and its Performance characteristics with various materials Design of Tunnel FET and its Performance characteristics with various materials 1 G.SANKARAIAH, 2 CH.SATHYANARAYANA 1 PG Student Sreenidhi Institute of Science and Technology, 2 Assistant Professor 1,

More information

General look back at MESFET processing. General principles of heterostructure use in FETs

General look back at MESFET processing. General principles of heterostructure use in FETs SMA5111 - Compound Semiconductors Lecture 11 - Heterojunction FETs - General HJFETs, HFETs Last items from Lec. 10 Depletion mode vs enhancement mode logic Complementary FET logic (none exists, or is likely

More information

NW-NEMFET: Steep Subthreshold Nanowire Nanoelectromechanical Field-Effect Transistor

NW-NEMFET: Steep Subthreshold Nanowire Nanoelectromechanical Field-Effect Transistor NW-NEMFET: Steep Subthreshold Nanowire Nanoelectromechanical Field-Effect Transistor Jie Xiang Electrical and Computer Engineering and Materials Science Engineering University of California, San Diego

More information

Alternatives to standard MOSFETs. What problems are we really trying to solve?

Alternatives to standard MOSFETs. What problems are we really trying to solve? Alternatives to standard MOSFETs A number of alternative FET schemes have been proposed, with an eye toward scaling up to the 10 nm node. Modifications to the standard MOSFET include: Silicon-in-insulator

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 11/01/2007 MOSFETs Lecture 5 Announcements HW7 set is due now HW8 is assigned, but will not be collected/graded. MOSFET Technology Scaling Technology

More information

Alternative Channel Materials for MOSFET Scaling Below 10nm

Alternative Channel Materials for MOSFET Scaling Below 10nm Alternative Channel Materials for MOSFET Scaling Below 10nm Doug Barlage Electrical Requirements of Channel Mark Johnson Challenges With Material Synthesis Introduction Outline Challenges with scaling

More information

EE 330 Lecture 7. Design Rules. IC Fabrication Technology Part 1

EE 330 Lecture 7. Design Rules. IC Fabrication Technology Part 1 EE 330 Lecture 7 Design Rules IC Fabrication Technology Part 1 Review from Last Time Technology Files Provide Information About Process Process Flow (Fabrication Technology) Model Parameters Design Rules

More information

Atomic-layer deposition of ultrathin gate dielectrics and Si new functional devices

Atomic-layer deposition of ultrathin gate dielectrics and Si new functional devices Atomic-layer deposition of ultrathin gate dielectrics and Si new functional devices Anri Nakajima Research Center for Nanodevices and Systems, Hiroshima University 1-4-2 Kagamiyama, Higashi-Hiroshima,

More information

45nm Bulk CMOS Within-Die Variations. Courtesy of C. Spanos (UC Berkeley) Lecture 11. Process-induced Variability I: Random

45nm Bulk CMOS Within-Die Variations. Courtesy of C. Spanos (UC Berkeley) Lecture 11. Process-induced Variability I: Random 45nm Bulk CMOS Within-Die Variations. Courtesy of C. Spanos (UC Berkeley) Lecture 11 Process-induced Variability I: Random Random Variability Sources and Characterization Comparisons of Different MOSFET

More information

Scaling of InGaAs MOSFETs into deep-submicron regime (invited)

Scaling of InGaAs MOSFETs into deep-submicron regime (invited) Scaling of InGaAs MOSFETs into deep-submicron regime (invited) Y.Q. Wu, J.J. Gu, and P.D. Ye * School of Electrical and Computer Engineering, Purdue University, West Lafayette, IN 47906 * Tel: 765-494-7611,

More information

Future MOSFET Devices using high-k (TiO 2 ) dielectric

Future MOSFET Devices using high-k (TiO 2 ) dielectric Future MOSFET Devices using high-k (TiO 2 ) dielectric Prerna Guru Jambheshwar University, G.J.U.S. & T., Hisar, Haryana, India, prernaa.29@gmail.com Abstract: In this paper, an 80nm NMOS with high-k (TiO

More information

Sustaining the Si Revolution: From 3D Transistors to 3D Integration

Sustaining the Si Revolution: From 3D Transistors to 3D Integration Sustaining the Si Revolution: From 3D Transistors to 3D Integration Tsu Jae King Liu Department of Electrical Engineering and Computer Sciences University of California, Berkeley, CA USA February 23, 2015

More information

Tunnel FET architectures and device concepts for steep slope switches Joachim Knoch

Tunnel FET architectures and device concepts for steep slope switches Joachim Knoch Tunnel FET architectures and device concepts for steep slope switches Joachim Knoch Institute of Semiconductor Electronics RWTH Aachen University Sommerfeldstraße 24 52074 Aachen Outline MOSFETs Operational

More information

HOW TO CONTINUE COST SCALING. Hans Lebon

HOW TO CONTINUE COST SCALING. Hans Lebon HOW TO CONTINUE COST SCALING Hans Lebon OUTLINE Scaling & Scaling Challenges Imec Technology Roadmap Wafer size scaling : 450 mm 2 COST SCALING IMPROVED PERFORMANCE 3 GLOBAL TRAFFIC FORECAST Cloud Traffic

More information

Band-Offset Engineering for GeSn-SiGeSn Hetero Tunnel FETs and the Role of Strain

Band-Offset Engineering for GeSn-SiGeSn Hetero Tunnel FETs and the Role of Strain Received 2 September 2014; revised 5 January 2015; accepted 8 January 2015. Date of current version 22 April 2015. The review of this paper was arranged by Editor A. C. Seabaugh. Digital Object Identifier

More information

3-D Modelling of the Novel Nanoscale Screen-Grid Field Effect Transistor (SGFET)

3-D Modelling of the Novel Nanoscale Screen-Grid Field Effect Transistor (SGFET) 3-D Modelling of the Novel Nanoscale Screen-Grid Field Effect Transistor (SGFET) Pei W. Ding, Kristel Fobelets Department of Electrical Engineering, Imperial College London, U.K. J. E. Velazquez-Perez

More information

Ultra High-Speed InGaAs Nano-HEMTs

Ultra High-Speed InGaAs Nano-HEMTs Ultra High-Speed InGaAs Nano-HEMTs 2003. 10. 14 Kwang-Seok Seo School of Electrical Eng. and Computer Sci. Seoul National Univ., Korea Contents Introduction to InGaAsNano-HEMTs Nano Patterning Process

More information

Nanotechnology, the infrastructure, and IBM s research projects

Nanotechnology, the infrastructure, and IBM s research projects Nanotechnology, the infrastructure, and IBM s research projects Dr. Paul Seidler Coordinator Nanotechnology Center, IBM Research - Zurich Nanotechnology is the understanding and control of matter at dimensions

More information

Fin-Shaped Field Effect Transistor (FinFET) Min Ku Kim 03/07/2018

Fin-Shaped Field Effect Transistor (FinFET) Min Ku Kim 03/07/2018 Fin-Shaped Field Effect Transistor (FinFET) Min Ku Kim 03/07/2018 ECE 658 Sp 2018 Semiconductor Materials and Device Characterizations OUTLINE Background FinFET Future Roadmap Keeping up w/ Moore s Law

More information

A new Hetero-material Stepped Gate (HSG) SOI LDMOS for RF Power Amplifier Applications

A new Hetero-material Stepped Gate (HSG) SOI LDMOS for RF Power Amplifier Applications A new Hetero-material Stepped Gate (HSG) SOI LDMOS for RF Power Amplifier Applications Radhakrishnan Sithanandam and M. Jagadesh Kumar, Senior Member, IEEE Department of Electrical Engineering Indian Institute

More information

MOS Capacitance and Introduction to MOSFETs

MOS Capacitance and Introduction to MOSFETs ECE-305: Fall 2016 MOS Capacitance and Introduction to MOSFETs Professor Peter Bermel Electrical and Computer Engineering Purdue University, West Lafayette, IN USA pbermel@purdue.edu 11/4/2016 Pierret,

More information

FinFET-based Design for Robust Nanoscale SRAM

FinFET-based Design for Robust Nanoscale SRAM FinFET-based Design for Robust Nanoscale SRAM Prof. Tsu-Jae King Liu Dept. of Electrical Engineering and Computer Sciences University of California at Berkeley Acknowledgements Prof. Bora Nikoli Zheng

More information

This Week s Subject. DRAM & Flexible RRAM. p-channel MOSFET (PMOS) CMOS: Complementary Metal Oxide Semiconductor

This Week s Subject. DRAM & Flexible RRAM. p-channel MOSFET (PMOS) CMOS: Complementary Metal Oxide Semiconductor DRAM & Flexible RRAM This Week s Subject p-channel MOSFET (PMOS) CMOS: Complementary Metal Oxide Semiconductor CMOS Logic Inverter NAND gate NOR gate CMOS Integration & Layout GaAs MESFET (JFET) 1 Flexible

More information

ECE520 VLSI Design. Lecture 2: Basic MOS Physics. Payman Zarkesh-Ha

ECE520 VLSI Design. Lecture 2: Basic MOS Physics. Payman Zarkesh-Ha ECE520 VLSI Design Lecture 2: Basic MOS Physics Payman Zarkesh-Ha Office: ECE Bldg. 230B Office hours: Wednesday 2:00-3:00PM or by appointment E-mail: pzarkesh@unm.edu Slide: 1 Review of Last Lecture Semiconductor

More information

Dopant Profiling of III-V Nanostructures for Electronic Applications

Dopant Profiling of III-V Nanostructures for Electronic Applications Dopant Profiling of III-V Nanostructures for Electronic Applications By Alexandra Caroline Ford A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy

More information

Wu Lu Department of Electrical and Computer Engineering and Microelectronics Laboratory, University of Illinois, Urbana, Illinois 61801

Wu Lu Department of Electrical and Computer Engineering and Microelectronics Laboratory, University of Illinois, Urbana, Illinois 61801 Comparative study of self-aligned and nonself-aligned SiGe p-metal oxide semiconductor modulation-doped field effect transistors with nanometer gate lengths Wu Lu Department of Electrical and Computer

More information

Sub-micron technology IC fabrication process trends SOI technology. Development of CMOS technology. Technology problems due to scaling

Sub-micron technology IC fabrication process trends SOI technology. Development of CMOS technology. Technology problems due to scaling Goodbye Microelectronics Welcome Nanoelectronics Sub-micron technology IC fabrication process trends SOI technology SiGe Tranzistor in 50nm process Virus The thickness of gate oxide= 1.2 nm!!! Today we

More information

Body-Biased Complementary Logic Implemented Using AlN Piezoelectric MEMS Switches

Body-Biased Complementary Logic Implemented Using AlN Piezoelectric MEMS Switches University of Pennsylvania From the SelectedWorks of Nipun Sinha 29 Body-Biased Complementary Logic Implemented Using AlN Piezoelectric MEMS Switches Nipun Sinha, University of Pennsylvania Timothy S.

More information

INTERNATIONAL JOURNAL OF APPLIED ENGINEERING RESEARCH, DINDIGUL Volume 1, No 3, 2010

INTERNATIONAL JOURNAL OF APPLIED ENGINEERING RESEARCH, DINDIGUL Volume 1, No 3, 2010 Low Power CMOS Inverter design at different Technologies Vijay Kumar Sharma 1, Surender Soni 2 1 Department of Electronics & Communication, College of Engineering, Teerthanker Mahaveer University, Moradabad

More information

Design and Analysis of Double Gate MOSFET Devices using High-k Dielectric

Design and Analysis of Double Gate MOSFET Devices using High-k Dielectric International Journal of Electrical Engineering. ISSN 0974-2158 Volume 7, Number 1 (2014), pp. 53-60 International Research Publication House http://www.irphouse.com Design and Analysis of Double Gate

More information

Silicon Single-Electron Devices for Logic Applications

Silicon Single-Electron Devices for Logic Applications ESSDERC 02/9/25 Silicon Single-Electron Devices for Logic Applications NTT Basic Research Laboratories Yasuo Takahashi Collaborators: : Yukinori Ono, Akira Fujiwara, Hiroshi Inokawa, Kenji Shiraishi, Masao

More information

Chapter 1. Introduction

Chapter 1. Introduction Chapter 1 Introduction 1.1 Introduction of Device Technology Digital wireless communication system has become more and more popular in recent years due to its capability for both voice and data communication.

More information

Near/Mid-Infrared Heterogeneous Si Photonics

Near/Mid-Infrared Heterogeneous Si Photonics PHOTONICS RESEARCH GROUP Near/Mid-Infrared Heterogeneous Si Photonics Zhechao Wang, PhD Photonics Research Group Ghent University / imec, Belgium ICSI-9, Montreal PHOTONICS RESEARCH GROUP 1 Outline Ge-on-Si

More information

Nanofluidic Diodes based on Nanotube Heterojunctions

Nanofluidic Diodes based on Nanotube Heterojunctions Supporting Information Nanofluidic Diodes based on Nanotube Heterojunctions Ruoxue Yan, Wenjie Liang, Rong Fan, Peidong Yang 1 Department of Chemistry, University of California, Berkeley, CA 94720, USA

More information

4.1.2 InAs nanowire circuits fabricated by field-assisted selfassembly on a host substrate

4.1.2 InAs nanowire circuits fabricated by field-assisted selfassembly on a host substrate 22 Annual Report 2010 - Solid-State Electronics Department 4.1.2 InAs nanowire circuits fabricated by field-assisted selfassembly on a host substrate Student Scientist in collaboration with R. Richter

More information

ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices

ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices Christopher Batten School of Electrical and Computer Engineering Cornell University http://www.csl.cornell.edu/courses/ece5950 Simple Transistor

More information

Innovative ultra-broadband ubiquitous Wireless communications through terahertz transceivers ibrow

Innovative ultra-broadband ubiquitous Wireless communications through terahertz transceivers ibrow Project Overview Innovative ultra-broadband ubiquitous Wireless communications through terahertz transceivers ibrow Mar-2017 Presentation outline Project key facts Motivation Project objectives Project

More information

Title. Author(s)Uemura, T.; Baba, T. CitationIEEE Transactions on Electron Devices, 49(8): Issue Date Doc URL. Rights.

Title. Author(s)Uemura, T.; Baba, T. CitationIEEE Transactions on Electron Devices, 49(8): Issue Date Doc URL. Rights. Title A three-valued D-flip-flop and shift register using Author(s)Uemura, T.; Baba, T. CitationIEEE Transactions on Electron Devices, 49(8): 1336-1 Issue Date 2002-08 Doc URL http://hdl.handle.net/2115/5577

More information

Semiconductor Nanowires for photovoltaics and electronics

Semiconductor Nanowires for photovoltaics and electronics Semiconductor Nanowires for photovoltaics and electronics M.T. Borgström, magnus.borgstrom@ftf.lth.se NW Doping Total control over axial and radial NW growth NW pn-junctions World record efficiency solar

More information

Session 10: Solid State Physics MOSFET

Session 10: Solid State Physics MOSFET Session 10: Solid State Physics MOSFET 1 Outline A B C D E F G H I J 2 MOSCap MOSFET Metal-Oxide-Semiconductor Field-Effect Transistor: Al (metal) SiO2 (oxide) High k ~0.1 ~5 A SiO2 A n+ n+ p-type Si (bulk)

More information

High-Speed Scalable Silicon-MoS 2 P-N Heterojunction Photodetectors

High-Speed Scalable Silicon-MoS 2 P-N Heterojunction Photodetectors High-Speed Scalable Silicon-MoS 2 P-N Heterojunction Photodetectors Veerendra Dhyani 1, and Samaresh Das 1* 1 Centre for Applied Research in Electronics, Indian Institute of Technology Delhi, New Delhi-110016,

More information

Improving CMOS Speed and Switching Energy with Vacuum-Gap Structures

Improving CMOS Speed and Switching Energy with Vacuum-Gap Structures Improving CMOS Speed and Switching Energy with Vacuum-Gap Structures Chenming Hu and Je Min Park Univ. of California, Berkeley -1- Outline Introduction Background and Motivation MOSFETs with Vacuum-Spacer

More information

Planarization and Regrowth of Self-Aligned Ohmic Contacts on InGaAs

Planarization and Regrowth of Self-Aligned Ohmic Contacts on InGaAs MBE 2008, Vancouver, B.C. Planarization and Regrowth of Self-Aligned Ohmic Contacts on InGaAs Mark Wistey, Greg Burek, Uttam Singisetti, Austin Nelson, Brian Thibeault, Joël Cagnon, Susanne Stemmer, Arthur

More information

ECE 340 Lecture 37 : Metal- Insulator-Semiconductor FET Class Outline:

ECE 340 Lecture 37 : Metal- Insulator-Semiconductor FET Class Outline: ECE 340 Lecture 37 : Metal- Insulator-Semiconductor FET Class Outline: Metal-Semiconductor Junctions MOSFET Basic Operation MOS Capacitor Things you should know when you leave Key Questions What is the

More information

Nanowire Tunnel Field Effect Transistors at High Temperature

Nanowire Tunnel Field Effect Transistors at High Temperature Nanowire Tunnel Field Effect Transistors at High Temperature Márcio D. V. Martino 1, Felipe S. Neves 1, Paula G. D. Agopian 1, João A. Martino 1, Rita Rooyackers 2 and Cor Claeys 2,3 1 LSI / PSI / USP

More information

ATV 2011: Computer Engineering

ATV 2011: Computer Engineering ATV 2011: Technology Trends in Computer Engineering Professor Per Larsson-Edefors ATV 2011, L1, Per Larsson-Edefors Page 1 Solid-State Devices www.cse.chalmers.se/~perla/ugrad/ SemTech/Lectures_2000.pdf

More information

Active Technology for Communication Circuits

Active Technology for Communication Circuits EECS 242: Active Technology for Communication Circuits UC Berkeley EECS 242 Copyright Prof. Ali M Niknejad Outline Comparison of technology choices for communication circuits Si npn, Si NMOS, SiGe HBT,

More information

International Association of Scientific Innovation and Research (IASIR) (An Association Unifying the Sciences, Engineering, and Applied Research)

International Association of Scientific Innovation and Research (IASIR) (An Association Unifying the Sciences, Engineering, and Applied Research) International Association of Scientific Innovation and Research (IASIR) (An Association Unifying the Sciences, Engineering, and Applied Research) International Journal of Emerging Technologies in Computational

More information

What is the highest efficiency Solar Cell?

What is the highest efficiency Solar Cell? What is the highest efficiency Solar Cell? GT CRC Roof-Mounted PV System Largest single PV structure at the time of it s construction for the 1996 Olympic games Produced more than 1 billion watt hrs. of

More information

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

ESE 570: Digital Integrated Circuits and VLSI Fundamentals ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 3: January 24, 2019 MOS Fabrication pt. 2: Design Rules and Layout Penn ESE 570 Spring 2019 Khanna Jack Keil Wolf Lecture http://www.ese.upenn.edu/about-ese/events/wolf.php

More information

SEVERAL III-V materials, due to their high electron

SEVERAL III-V materials, due to their high electron IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 64, NO. 1, JANUARY 2017 239 Gate Bias and Geometry Dependence of Total-Ionizing-Dose Effects in InGaAs Quantum-Well MOSFETs Kai Ni, Student Member, IEEE, En Xia

More information

2009 Spring CS211 Digital Systems & Lab 1 CHAPTER 3: TECHNOLOGY (PART 2)

2009 Spring CS211 Digital Systems & Lab 1 CHAPTER 3: TECHNOLOGY (PART 2) 1 CHAPTER 3: IMPLEMENTATION TECHNOLOGY (PART 2) Whatwillwelearninthischapter? we learn in this 2 How transistors operate and form simple switches CMOS logic gates IC technology FPGAs and other PLDs Basic

More information

Research Needs for Device Sciences Modeling and Simulation (May 6, 2005)

Research Needs for Device Sciences Modeling and Simulation (May 6, 2005) Research Needs for Device Sciences Modeling and Simulation (May 6, 2005) SRC Device Sciences 2005 Modeling and Simulation Task Force Contributing organizations: Axcelis, Freescale, IBM, Intel, LSI, SRC,

More information

Towards a Reconfigurable Nanocomputer Platform

Towards a Reconfigurable Nanocomputer Platform Towards a Reconfigurable Nanocomputer Platform Paul Beckett School of Electrical and Computer Engineering RMIT University Melbourne, Australia 1 The Nanoscale Cambrian Explosion Disparity: Widerangeof

More information

Performance Evaluation of MISISFET- TCAD Simulation

Performance Evaluation of MISISFET- TCAD Simulation Performance Evaluation of MISISFET- TCAD Simulation Tarun Chaudhary Gargi Khanna Rajeevan Chandel ABSTRACT A novel device n-misisfet with a dielectric stack instead of the single insulator of n-mosfet

More information

NAME: Last First Signature

NAME: Last First Signature UNIVERSITY OF CALIFORNIA, BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences EE 130: IC Devices Spring 2003 FINAL EXAMINATION NAME: Last First Signature STUDENT

More information